1. Consider a scalar space ψ.
  • ψ and ψ’ represent the same 4-vector input regardless of the frame.
  • (Of course, if it’s a different frame, it’s a different event, but we won’t consider that here.)
  1. Relate the position dependence of the fields between the two frames.
  • It is important not to mix up these issues.

  • The surface charge density is equal to ρ times d.

    • If we boost in the direction perpendicular to the surface, ρ will change but d will remain constant.
    • E, which is proportional to the density (e.g. σ/2ε_0), is not a 4-vector.
    • The component in the boost direction is invariant.

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  • There are cases where ρ=0 and J=0.

    • J=0 means there is charge but the velocity is zero.
    • ρ=0 refers to something magnetic.
  • Transformation of Gauss’s law

    • The partial derivative interacts with the Lorentz contact and introduces a γ factor.
  • Towards the end

    • I want to verify the conditions ∇・E = 0 and J = 0.